DIFFUSED PHASE-TRANSITION IN PB-0.91(LA1-Z 3,LI-Z)(0.09)(ZR0.65TI0.35)(0.9775)O-3 CERAMICS/

Citation
Hr. Rukmini et al., DIFFUSED PHASE-TRANSITION IN PB-0.91(LA1-Z 3,LI-Z)(0.09)(ZR0.65TI0.35)(0.9775)O-3 CERAMICS/, Journal of physics and chemistry of solids, 59(9), 1998, pp. 1541-1548
Citations number
12
Categorie Soggetti
Physics, Condensed Matter",Chemistry
ISSN journal
00223697
Volume
59
Issue
9
Year of publication
1998
Pages
1541 - 1548
Database
ISI
SICI code
0022-3697(1998)59:9<1541:DPIP3>2.0.ZU;2-X
Abstract
The sol-gel process was used to prepare lithium-modified polycrystalli ne PLZT, Pb-0.91(La1-z/3, Li-z)(0.09)(Zr0.65Ti0.35)(0.9775)O-3 (z = 0 0. 0.1. 0.3, 0.5, 0.7] (PLLZT), near the morphotropic phase boundary. X-ray diffraction studies of these compounds suggest that they can be formed in single phase at relatively low temperatures (similar to 800 degrees C). The green pellets of these compounds were sintered at 1100 degrees C. Detailed studies of the dielectric constant (epsilon) and loss tangent (tan delta) of PLLZT ceramics as a function of temperatur e (room temperature to 350 degrees C) at 1 and 10 kHz frequencies sugg est that the compounds exhibit relaxer behaviour and undergo ferroelec tric phase transition of diffuse type on increasing the lithium concen tration. Analysis of the broadened dielectric peaks of these compounds provided values of diffusivity (gamma) between 1 and 2, which indicat es the variation in the degree of disordering with change in z. The tr ansition temperature (T-C) of the compounds was found to increase with increasing lithium concentration. The variation in the values of diel ectric constant (epsilon) and loss tangent (tan delta) with lithium co ncentration shows very interesting behaviour of the compounds. The ele ctrical conductivity and the activation energy of PLLZT provided some interesting results. (C) 1998 Elsevier Science Ltd. All rights reserve d.